论文标题
黑洞的旋转积聚盘中的旋转进化
Black hole spin evolution in warped accretion discs
论文作者
论文摘要
居住在银河系核的巨大黑洞(BHS)只能通过两个参数(即质量和自旋)来描述,这些参数会因响应增生和合并事件而变化。虽然大多数数值模拟可以准确地跟踪BH质量,但很少考虑自旋进化。在这项工作中,我们实施并验证了BH质量演化的自洽子网模型,并在流体力学代码Gizmo中通过气体积聚旋转。该模型假设从分辨率量表中的积聚不会立即发生,而是由亚网格几何薄$α$ disc介导的。在半分析验证我们的模型后,我们在由环核盘组成的理想化环境中进行测试,在该环境中,在该圆盘中,在该盘中,在该盘上,在该环境中,浓积盘上的气体积聚始终由Gizmo确定。在没有任何吸积相关的反馈的情况下,旋转进化在半分析模型中观察到的痕迹取决于我们实施的自由参数,例如初始BH旋转,积聚盘的角动量以及气体流入循环的半径。在Gizmo中,我们还将模型与伴侣纸中呈现的双色散流模型相结合,其中反馈轴始终与BH旋转对齐。在最后一个情况下,中央BH的演变与以前的情况有显着不同,因为反馈过程会改变了气体动力学及其从分辨率量表中的流入率。这种相互作用不能通过简单的半分析模型来建模,应使用全n体流体动力学模拟对其进行处理。
Massive black holes (BHs) inhabiting galactic nuclei can be described by two parameters only, i.e. mass and spin, that change through cosmic time in response to accretion and merger events. While most numerical simulations accurately track the BH mass, spin evolution is rarely taken into account. In this work, we implement and validate a self-consistent sub-grid model for the evolution of the BH mass and spin via gas accretion in the hydrodynamics code GIZMO. The model assumes that accretion from resolved scales does not occur instantaneously, but is mediated by a sub-grid geometrically thin $α$-disc. After validating our model semi-analytically, we test it in an idealized environment consisting of a circumnuclear disc, where gas accretion onto the accretion disc is consistently determined by GIZMO. In the absence of any accretion-related feedback, the spin evolution closely traces that observed in the semi-analytical models and depends on the free parameters of our implementation, such as the initial BH spin, angular momentum of the accretion disc, and the radius at which the gas inflow circularises. In GIZMO, we also couple our model with the biconical-outflow model presented in a companion paper, wherein the feedback axis is always aligned with the BH spin. In this last case, the evolution of the central BH differs significantly from the previous cases, since the feedback process modifies the gas dynamics and its inflow rates from resolved scales. Such an interaction cannot be modeled by simple semi-analytical models and should be treated using full N-body hydrodynamical simulations.